Durable sputtered metal oxide coating

Abstract: A method and resultant product are disclosed wherein a metal film is deposited by sputtering a metal cathode target in an essentially nonreactive atmosphere comprising inert gas and a reactive gas, wherein the concentration of reactive gas is sufficiently low that the sputtering is accomplished in the metallic mode, i.e. the film is deposited as metal. The metal film of the present invention is harder than a metal film sputtered in an atmosphere consisting of only inert gas. The method and resultant product may further comprise thermal oxidation of the metal film, which proceeds more efficiently than oxidation of a metal film sputtered in an atmosphere consisting of only inert gas.

Description: The present invention relates generally to the art of sputtered films and more particularly to the art of durable metal oxide films produced by magnetron sputtering. Sputtered metal oxide films are well known in the art. Tin oxide, zinc oxide, titanium oxide and many other metal oxides are known to be deposited by sputtering the respective metals in an oxidizing atmosphere such as air or a mixture of oxygen and inert gas such as argon. It is also known that a metal film can be deposited by sputtering a metal in an inert atmosphere such as argon, and the metal film subsequently oxidized thermally by heating in an oxidizing atmosphere such as air. Various metals can be deposited either as metallic films or metal oxide films depending on whether the metal cathode target is sputtered in an inert atmosphere or an oxidizing atmosphere. Generally, sputtering in an inert atmosphere, i.e. in the metallic mode, is faster and more efficient. The resulting coating is a metal film having metallic properties, i.e. generally low transmittance, high reflectance and electrically conductive. Such films are generally not very hard or durable, and are easily damaged in handling. Dielectric metal oxide films are typically high transmittance, lower reflectance and electrically insulating. However, because they are insulating, they do not deposit as efficiently by sputtering. To produce very thick metal oxide films by sputtering is inefficient, costly and may not result in a durable film. To produce very thick metal oxide films by thermally oxidizing metal films efficiently sputtered in an inert atmosphere is inherently rate-limited because oxygen may not readily penetrate beyond the initially formed surface layer of metal oxide. M. Yoshitake et al. reported in "Thin Solid Films" 230(1993)July 15, No. 1, p.48-54, on the use of ion beam current as a process control in the reactive sputtering of zirconium oxide. It is disclosed that the oxygen partial pressure changes greatly from the initial oxygen pressure when sputtering zirconium in an oxygen atmosphere. Because Zr is a very active element, as is Ti, these sputtered Zr atoms capture O 2 molecules by gettering action. The transmission characteristics of several Zr-O films deposited on a fused quartz substrate at a constant O 2 pressure are reported. The film deposited at an I B of 110 mA is metallic and no transmitted light was observed. No transparent film were obtained in the I B region between 40 and 110 mA, when sputtering at pressures below 2.7 x 10 -3 Pa. For the preparation of Zr-O films at a constant P o , the crystal structure, composition, and optical and electrical properties are all influenced by I B . In the high I B region, Zr atoms are sputtered and Zr films that include oxygen atoms but have metallic properties are deposited. K.G. Geraghty and L.F. Donaghey reported on kinetics of the reactive sputter deposition of titanium oxides in the Journal of the Electrochemical Society, Vol.123,No.8, August 1976, p.1201-1207. It is mentioned that a critical oxygen partial pressure exists in the plasma, p O2 *, below which no oxidation of the target takes place. For p O2 > p O2 *, the sputter rate exceeds the oxidation rate and no oxidation layer is formed on the target. However, these experimental results of Heller are not inconsistent with the study of Greiner. The authors of said publication performed sputtering in the range of oxygen mole fraction y ranging from 0 to 0.15. Titanium was sputtered in pure argon (y = 0) as a standard for comparison in assessing the effects of O 2 on sputtering parameters. A significant transition in density and deposition rate was observed at an oxygen mole fraction y*= 0.007. The rapid etching characteristics of reactively sputtered TiO x films with x < 2 suggests that the films are amorphous. Films deposited at very low y (≤ 0.002) were metallic and showed same visible absorbance. The study of the reactive sputter deposition rates of titanium oxides shows that amorphous films were deposited at room temperature over the entire range of mole fractions studied. Deposited films were generally metallic α Ti for oxygen mole fractions y < 0.002, and dielectric TiO 2 for y < 0.035. From McGraw-Hill, Encyclopedia of Science and Technology, 5 th Edition, p.748 it is known that metallic α Ti films are crystalline. It is the object of the invention to provide a process for depositing a sputtered hard metal film which is oxidizable into a chemical durable metal oxide film. This object is attained by a method of depositing a hard metal film onto a substrate by cathode sputtering comprising the steps of: a. placing the substrate in an evacuated chamber having a metal cathode target and comprising an atmosphere comprising argon as inert gas and an amount of from 2 to 30 percent oxygen as reactive gas, and b. sputtering with power levels of 2 to 4 kilowatts the metal cathode target and depositing a metal film having a thickness in the range of 10 nm to 150 nm (100 to 1500 Angstroms), while controlling the amount of reactive gas in the atmosphere below the switching point from the metallic sputtering mode to the oxide sputtering mode, so that the metal is sputtered in the metallic mode, but the amount of reactive gas is sufficient such that the metal film deposited is substantially amorphous rather than crystalline, so that the amorphous metal film has a higher transmission and is harder and less dense than a crystalline metal film sputtered in pure argon. The solution includes a method of depositing a metal oxide film onto a substrate by depositing a hard metal film onto the substrate by cathode sputtering comprising the steps of: a. placing the substrate in an evacuated chamber having a metal cathode target and comprising an atmosphere comprising argon as inert gas and an amount of from 2 to 30 percent oxygen as reactive gas, and b. sputtering with power levels of 2 to 4 kilowatts the metal cathode target to deposit a metal film having a thickness in the range of 10 nm to 150 nm (100 to 1500 Angstroms), while controlling the amount of reactive gas in the atmosphere below the switching point from the metallic sputtering mode to the oxide sputtering mode, so that the metal is sputtered in the metallic mode, but the amount of reactive gas is sufficient such that the metal film deposited is substantially amorphous rather than crystalline, so that the amorphous metal film has a higher transmission and is harder and less dense than a crystalline metal film sputtered in pure argon, and c. thermally oxidizing the metal film in a further step. The amorphous sputtered metal film is harder and more durable than a metal film sputtered in an atmosphere consisting of only inert gas. The amorphous sputtered metal film may be thermally oxidized more efficiently than a metal film deposited in an atmosphere consisting of only inert gas, resulting in a crystalline metal oxide film which is substantially more chemically durable than an amorphous metal oxide film deposited by sputtering metal in an oxidizing atmosphere. DESCRIPTION OF THE DRAWING Figure 1 illustrates the maximum percentage of oxygen in inert gas which allows sputtering of titanium in the metallic mode using an AIRCO ILS-1600 laboratory scale coater as a function of power level in kilowatts (kw). Figure 2 illustrates the maximum percentage of oxygen in inert gas which allows sputtering of zirconium in the metallic mode using an AIRCO ILS-1600 laboratory scale coater as a function of power level in kw. Figure 3 illustrates the voltage as a function of percent oxygen in inert gas for the sputtering of titanium at power levels of 1, 2, 3 and 4 kilowatts using an AIRCO ILS-1600 laboratory scale coater. The peak on each curve is the switching point where the amount of oxygen causes the sputtering mode to change from the metal mode to the oxide mode. Metals such as titanium, zirconium, tantalum, hafnium, niobium, vanadium and mixtures thereof, preferably titanium and zirconium, may be deposited in a substantially amorphous metallic state in accordance with the present invention by sputtering the metal in a nonreactive atmosphere substantially comprising argon as inert gas, but also comprising 2-30% oxygen as reactive gas. The amount of oxygen is sufficient to effect the deposition of the metal in a substantially amorphous rather than crystalline state, but insufficient to effect the transition of sputtering from the metallic mode to the oxide mode. The appropriate amount of oxygen in the inert gas for purposes of the present invention is related to the cathode operating parameters, particularly the power, and the size of the target. Figures 1 and 2 illustrate the maximum oxygen concentration in argon at various levels of power for titanium and zirconium targets respectively operated in an AIRCO ILS-1600 laboratory scale coater. At higher oxygen concentrations, the sputtering mode will switch from metallic to oxide, resulting in the slow deposition of amorphous metal oxide. Therefore, the oxygen concentration is kept sufficiently low to avoid depositing metal oxide. However, it has been discovered that the higher the oxygen concentration, below the switching point, the harder the amorphous metal deposited in the metal sputtering mode. Figure 3 illustrates the voltage as a function of oxygen concentration for titanium films deposited at power levels of from 1 to 4 kilowatts in an AIRCO ILS-1600 laboratory scale coater. The voltage peak for each curve illustrates the switching point between metallic and oxide sputtering modes, and indicates the maximum oxygen concentration for the specified power level using this coating apparatus. It is preferred to operate near the peak, i.e. at a relatively higher concentration of oxygen, for maximum metal hardness, but without switching from the metallic sputtering mode to the oxide sputtering mode. The amorphous metal film sputtered in an oxygen-containing but substantially nonreactive atmosphere is only slightly higher in transmission than a metal film sputtered in pure argon; and the sputtering rate is approximately the same. However, the amorphous metal coating sputtered in an oxygen-containing but substantially nonreactive atmosphere is significantly harder and less dense than a crystalline metal film sputtered in pure argon. The relative hardness of such metal films is determined by abrasion of the film followed by visual examination and rating on the basis of film damage. A method of judging the hardness of metal films comprises repeated strokes of an abrasive pad (Scotch-Brite® 98 Light Duty Cleaning Pad from 3M) followed by visual examination on a light board and rating the film damage on a scale of 1 to 9, with 1 being insignificant damage and 9 being substantial removal of the metal film. The density of amorphous titanium metal film sputtered in an essentially nonreactive atmosphere comprising inert gas and 10 percent oxygen is 4.0 grams per cubic centimeter (g/cm 3 ), compared with a density of 4.5 g/cm 3 for a titanium metal film sputtered in pure argon. The lower density of the amorphous titanium metal film enhances its rate of oxidation, so that the amorphous titanium metal film may be thoroughly oxidized at lower temperatures and/or in shorter times than required for oxidation of crystalline titanium metal film. The hard, dense, amorphous metal coating of the present invention in a thickness range of 0.01 µm to 0.15 µm (100 to 1500 Angstroms), more preferably 0.02 µm to 0.1 µm (200 to 1000 Angstroms) for titanium, is sufficiently durable to withstand handling, shipping and processing, such as heat strengthening, tempering and bending. It is preferred to further process the amorphous metal film of the present invention by thermally oxidizing the metal to metal oxide. The hard amorphous metal film of the present invention may be thermally oxidized to metal oxide by heating to produce a haze-free, dense, substantially crystalline metal oxide coating which is sufficiently chemically and physically durable to be coated on the exposed surface of a glass substrate. The amorphous metal film is preferably heated to a temperature of at least 400°C, preferably 500 to 700°C, in air in order to effect complete oxidation in a reasonable time, e.g. a few minutes. The method of the present invention of heating an amorphous sputtered metal film to produce a crystalline metal oxide film is a more efficient method to produce thick metal oxide films than reactively sputtering such films. Moreover, the crystalline thermally oxidized metal oxide films are more chemically durable than the substantially amorphous reactively sputtered metal oxide films. Such crystalline thermally oxidized metal oxide films may be produced over a wide range of thicknesses having a wide range of desirable reflected colors produced by interference effects. The density of the titanium oxide coatings is determined using the measured thickness of the coating and the weight percent titanium in fully oxidized titanium oxide. The thickness was measured using a Tencor P-1 Long Scan Profiler; the weight percent titanium was measured using x-ray fluorescence. The density of the crystalline thermally oxidized titanium coating is greater than the density of amorphous reactively sputtered titanium dioxide coating; the crystalline thermally oxidized titanium oxide coating has a density of 4.0 grams per cubic centimeter (g/cm 3 ) while the amorphous sputtered titanium oxide has a density of 3.4 g/cm 3 . The density of crystalline thermally oxidized titanium oxide coatings approaches the bulk density of 4.26 g/cm 3 for the rutile phase of TiO 2 . The refractive index at 600 nanometers of an amorphous reactively sputtered titanium oxide film is 2.3, whereas the refractive index at 600 nanometers of a crystalline titanium oxide film thermally oxidized from an amorphous titanium metal film sputtered in an essentially nonreactive atmosphere comprising argon and 10 percent oxygen is 2.5, which is nearly the refractive index of the rutile phase of bulk crystalline TiO 2 . In a preferred embodiment of the present invention, coatings are produced on a large-scale magnetron sputtering device capable of coating glass up to (100 x 144 inches) 2.54 x 3.66 meters . Using a commercial production scale coater, the acceptable amount of reactive gas may be considerably higher without switching from the metal mode compared with a small-scale coater, particularly if multiple cathodes are sputtered simultaneously within a chamber at higher power density. In the following examples, the coatings are deposited on a smaller scale, using planar magnetron cathodes having(5 x 17 inch) 12.7 x 43.2 centimeters targets. Base pressure is in the 0.133 x 10 -3 Pa (10 -6 Torr) range. The coatings are made by first admitting the sputtering gas to a pressure of 0.532 Pa (4 microns Hg) and then setting the cathode power. In each example, glass substrates pass under the target on a conveyor roll at a speed of (120 inches) 3.05 meters per minute. The transmittance is monitored every other pass during the sputtering process at a wavelength of 550 nanometers using a Dyn-Optics 580D optical monitor. After the coating is deposited, the transmittance and reflectance from both the glass and coated surfaces are measured in the wavelength range from 380 to 720 nanometers using Pacific Scientific Spectrogard Color System spectrophotometer. In a most preferred embodiment of the present invention, the amorphous metal film sputtered in an essentially nonreactive atmosphere comprising sufficient oxygen as reactive gas to effect the deposition of a harder, less dense, amorphous, rather than crystalline, metal film, but insufficient to effect the transition of the sputtering process from the metallic to the oxide mode, is overcoated with a thin layer of reactively sputtered amorphous metal oxide. This layer of reactively sputtered amorphous metal oxide increases the thermal stability of the amorphous metal film sputtered in an essentially nonreactive atmosphere comprising argon as inert gas and sufficient oxygen as reactive gas to effect the deposition of an amorphous metal film but insufficient to effect the transition of the sputtering mode from metallic to oxide, during thermal oxidation. The amorphous sputtered metal oxide layer preferably comprises the same metal as the underlying amorphous metal layer. The thickness of the amorphous metal oxide layer is preferably in the range of 0.004 µm-0.012 µm (40 to 120 Angstroms). The thickness of the underlying amorphous metal layer is preferably in the range of 0.02 µm to 0.1 µm (200 to 1000 Angstroms) prior to thermal oxidation, for production of a wide range of chromas in the metal oxide films. The amount of oxygen in the essentially nonreactive atmosphere may vary widely depending on the metal to be sputtered, size and geometry of targets, number and power level of cathodes, and so on. The upper limit in any case is below the point at which sputtering switches from the metallic to the oxide mode. For optimum hardness of the amorphous metal film, it is preferred to operate near this upper limit consistent with maintaining sputtering in the metal mode. A range of 2 to 30 percent oxygen, preferably 5 to 25 percent may be preferred when sputtering titanium. The present invention will be further understood from the descriptions of specific examples which follow. EXAMPLE 1 A clear glass substrate six millimeters thick was coated with titanium as follows. A titanium cathode target was sputtered in an atmosphere of argon containing 2.5 percent oxygen. The base pressure was 0.266 x 10 -3 Pa (2 X 10 -6 Torr), operating pressure 0.532 Pa (4.0 µm Hg). Power was set at 3.0 kilowatts (kw), voltage was 381 volts (V), current was 7.8 amps and line speed (120 inches) 3.05 meters , per minute. After 1 pass, the transmittance was 19.1 percent, after three passes 2.0 percent, and zero after four passes. The resistance of the titanium film was 41.9 ohms per square. The coated surface was wiped with an abrasive pad (Scotch-Brite from 3M), and the coated substrate placed on a light board for visual examination. It was rated 7 in transmittance and 5 in reflectance. EXAMPLE 2 A glass substrate was coated as in Example 1 except that the atmosphere was argon with 5 percent oxygen, the voltage was 385V and the current 7.7 amps. The transmittance after one pass was 21.0 percent, after three passes 2.6 percent, and less than one percent after four passes. The resistance of the titanium film was 48 ohms per square. The coated surface was rated 5 in transmittance and 4 in reflectance after abrasion. EXAMPLE 3 A glass substrate was coated as in Examples 1 and 2 except that the atmosphere was argon with 10 percent oxygen, the voltage was 393V and the current 7.6 amps. The transmittance after one pass was 26.4 percent, after three passes 6.0 percent, and 2.0 percent after four passes. The resistance of the titanium film was 82 ohms per square. The coated surface was rated 2 in both transmittance and reflectance after abrasion. EXAMPLE 4 A glass substrate was coated as in the previous examples except that the atmosphere contained 15 percent oxygen, the voltage was 432V and the current 6.9 amps. The transmittance after one pass was 57.0 percent, after three passes 21.0 percent, and 13.6 percent after four passes. The resistance of the titanium film was 330 ohms per square. The coated surface was rated 1 in both transmittance and reflectance after abrasion. The increasing transmittance and resistance indicate that the oxygen concentration is approaching the maximum for sputtering in the metal mode, although the film is still metallic, since the resistance is still very low in comparison with the resistance of titanium oxide, which is infinite, i.e. titanium oxide is an insulating material. COMPARATIVE EXAMPLE A A-glass substrate was coated as in the previous examples except that the atmosphere was pure argon, the voltage was 378V and the current 7.85 amps. The transmittance after one pass was 18.0 percent, after three passes 1.8 percent, and zero after four passes. The resistance of the titanium film was 24 ohms per square. The coated surface was rated 9 in both transmittance and reflectance after abrasion. EXAMPLE 5 A tinted glass (SOLEX® glass from PPG Industries, Inc.) substrate 4.0 millimeters thick was coated with titanium and titanium dioxide as follows. The first layer of coating is prepared by sputtering a planar titanium cathode in an atmosphere of argon containing 10 percent oxygen. The base pressure was 0.93 x 10 -3 Pa (7.0 x 10 -6 Torr), operating pressure 0.532 Pa (4.0 µm Hg), power set at 3.4 kilowatts, voltage was 399 volts, current 8.42 amps and line speed (120 inches) 3.05 meters per minute. After 4 passes, the transmittance was 1.4 percent. The titanium layer thickness was 0.0599 µm (599 Angstroms). This layer deposition was followed by reactively sputtering titanium in a 50/50 argon/oxygen gas mixture. Power was set at 5.0 kilowatts, voltage was 470 volts, current 10.57 amps and the line speed (120 inches) 3.05 meters per minute. After 6 passes, the final transmittance was 2.0 percent. The coating thickness for the reactively sputtered titanium oxide layer was 0.0076 µm (76 Angstroms). The two layer coating was then heated for 4 minutes to a temperature of 650°C, producing a single homogeneous layer of titanium oxide coating with thickness of 0.106 µm (1062 Angstroms). The optical properties of the coated article were analyzed and are shown in the Table following the Examples. EXAMPLE 6 A clear glass substrate 6.0 millimeters thick was coated with titanium as follows. A coating was prepared by sputtering a planar titanium cathode in an atmosphere of argon containing 10 percent oxygen. The base pressure was 0.785 x 10 -3 Pa (5.9 x 10 - 6 Torr) operating pressure 0.532 Pa (4.0 µm Hg), power set at 3.4 kilowatts, voltage was 398 volts, current 8.45 amps and line speed (120 inches) 3.05 meters per minute. After 6 passes the transmittance was zero. The coating thickness was 0.0893 µm (893 Angstroms). The coating was then heated for 6.5 minutes to a temperature of 637°C producing an oxide coating with a thickness of 0.1469 µm (1469 Angstroms). The optical properties are shown in the Table following the Examples. EXAMPLE 7 A clear glass substrate 6.0 millimeters thick was coated with titanium as follows. A coating was prepared by sputtering a planar titanium cathode in an atmosphere of argon containing 10 percent oxygen. The base pressure was 0.665 x 10 -3 Pa (5.0 x 10 - 6 Torr), operating pressure 0,532 Pa (4.0 µm Hg), power set at 3.4 kilowatts, voltage was 398 volts, current 8.45 amps and line speed (120 inches) 3.05 meters per minute. After 5 passes the transmittance was 0.5 percent. The coating thickness was 0.0742 µm (742 Angstroms). The coating was then heated for 6.5 minutes to a temperature of 637°C, producing an oxide coating with a thickness of 0.122 µm (1220 Angstroms). The optical properties are shown in the Table following the Examples. EXAMPLE 8 A clear glass substrate 6.0 millimeters thick was coated with titanium as follows. A coating was prepared by sputtering a planar titanium cathode in an atmosphere of argon containing 10 percent oxygen. The base pressure was 0.52 x 10 -3 Pa (3.9 x 10 - 6 Torr) operating pressure 0.532 Pa (4.0 µm Hg), power was set at 3.4 kilowatts, voltage was 398 volts, current 8.45 amps and line speed (120 inches) 3.05 meters per minute. After 4 passes the transmittance was 1.6 percent. The coating thickness was 0.0599 µm (599 Angstroms). The coating was then heated for 6.5 minutes to a temperature of 637°C, producing an oxide coating with a thickness of 0.0986 µm (986 Angstroms). The optical properties are shown in the Table following the Examples. EXAMPLE 9 A clear glass substrate 6.0 millimeters thick was coated with titanium as follows. A coating was prepared by sputtering a planar titanium cathode in an atmosphere of argon containing 10 percent oxygen. The base pressure was 0.78 x 10 -3 Pa (5.9 x 10 - 6 Torr), operating pressure 0.532 Pa (4.0 µm Hg), power was set at 3.4 kilowatts, voltage was 398 volts, current 8.45 amps and line speed (120 inches) 3.05 meters per minute. After 3 passes the transmittance was 3.9 percent. The coating thickness was 0.0477 µm (447 Angstroms). The coating was then heated for 6.5 minutes to a temperature of 637°C, producing an oxide coating with a thickness of 0.0735µm (735 Angstroms). The optical properties are shown in the Table following the Examples. EXAMPLE 10 A clear glass substrate 6.0 millimeters thick was coated with titanium as follows. A coating was prepared by sputtering a planar titanium cathode in an atmosphere of argon containing 10 percent oxygen. The base pressure was 0.69 x 10 -3 Pa (5.2 x 10 - 6 Torr), operating pressure 0.532 Pa (4.0 µm Hg), power was set at 3.4 kilowatts, voltage was 398 volts, current 8.45 amps and line speed (120 inches) 3.05 meters per minute. After 2 passes the transmittance was 8.9 percent. The coating thickness was 0.0301 µm (301 Angstroms). The coating was then heated for 6.5 minutes to a temperature of 637°C, producing an oxide coating with thickness of 0.0495 µm (495 Angstroms). The optical properties are shown in the Table following the Examples. EXAMPLE 11 A tinted glass (SOLEX® glass from PPG Industries, Inc.) substrate 4.0 millimeters thick was coated with titanium as follows. A coating was prepared by sputtering a planar titanium cathode in an atmosphere of argon containing 10 percent oxygen. The base pressure was 0.93 x 10 -3 Pa (7.0 x 10 -6 Torr), operating pressure 0,532 Pa (4.0 µm Hg), power was set at 3.4 kilowatts, voltage was 400 volts, current 8.4 amps and line speed (120 inches) 3.05 meters per minute. After 4 passes the transmittance was 1.5 percent. The coating thickness was 0.0599 µm (599 Angstroms). The coating was then heated for 4 minutes to a temperature of 650°C, producing an oxide coating with thickness of 0.0981 µm (986 Angstroms). The optical properties are shown in the Table following the Examples. Transmittance Reflectance Example # Film Side Glass Side Y x y Y x y Y x y 5 74.46 .3102 .3646 12.25 .3038 .2152 10.34 .3032 .2286 6 65.71 .3444 .3373 30.43 .2418 .3182 28.94 .2412 .3209 7 82.90 .3451 .3792 13.23 .2056 .1833 12.82 .2074 .1884 8 79.31 .2968 .3374 17.33 .3733 .3072 16.37 .3679 .3105 9 60.37 .2897 .3022 36.54 .3574 .3914 34.31 .3502 .3922 10 56.63 .3205 .3374 40.09 .2985 .3205 37.76 .2940 .3224 11 72.15 .2925 .3398 17.51 .3794 .3165 14.73 .3652 .3264 The above examples are offered to illustrate the present invention. Other metals such as zirconium, tantalum, vanadium, hafnium and niobium may be sputtered in an atmosphere which contains oxygen as reactive gas but which remains essentially nonreactive. The amount of oxygen as reactive gas is kept sufficiently low so that the sputtering mode is essentially metallic, and the film deposited is essentially metallic. To optimize the hardness of the metal film, the amount of oxygen in the inert gas is preferably as high as is consistent with maintaining an essentially nonreactive atmosphere, i.e. sputtering in the metallic mode. The reactive gas is oxygen, the minimum amount is sufficient to effect deposition of amorphous metal, generally at least 2 percent, and higher amounts, at least about 10 percent, are preferred in order to thermally oxidize at an efficient rate. Thermal oxidation of the metallic film may be performed throughout a range of temperatures sufficient to oxidize the metal without deteriorating the integrity of the film. Typically, a temperature of at least 400°C is selected to thoroughly oxidize the metal film in a reasonable time, e.g. a few minutes. Film thicknesses may vary over a wide range to obtain desirable properties, particularly interference color effects in reflectance.

Claims: A method of depositing a hard metal film onto a substrate by cathode sputtering comprising the steps of: a. placing the substrate in an evacuated chamber having a metal cathode target and comprising an atmosphere comprising argon as inert gas and an amount of from 2 to 30 percent oxygen as reactive gas, and b. sputtering with power levels of 2 to 4 kilowatts the metal cathode target and depositing a metal film having a thickness in the range of 10 nm to 150 nm (100 to 1500 Angstroms), while controlling the amount of reactive gas in the atmosphere below the switching point from the metallic sputtering mode to the oxide sputtering mode, so that the metal is sputtered in the metallic mode, but the amount of reactive gas is sufficient such that the metal film deposited is substantially amorphous rather than crystalline, so that the amorphous metal film has a higher transmission and is harder and less dense than a crystalline metal film sputtered in pure argon. The method according to claim 1, wherein the metal cathode target is selected from the group consisting of titanium, zirconium, tantalum, hafnium, niobium, vanadium and mixtures thereof. A method of depositing a metal oxide film onto a substrate by depositing a hard metal film onto the substrate by cathode sputtering comprising the steps of: a. placing the substrate in an evacuated chamber having a metal cathode target and comprising an atmosphere comprising argon as inert gas and an amount of from 2 to 30 percent oxygen as reactive gas, and b. sputtering with power levels of 2 to 4 kilowatts the metal cathode target to deposit a metal film having a thickness in the range of 10 nm to 150 nm (100 to 1500 Angstroms), while controlling the amount of reactive gas in the atmosphere below the switching point from the metallic sputtering mode to the oxide sputtering mode, so that the metal is sputtered in the metallic mode, but the amount of reactive gas is sufficient such that the metal film deposited is substantially amorphous rather than crystalline, so that the amorphous metal film has a higher transmission and is harder and less dense than a crystalline metal film sputtered in pure argon, and c. thermally oxidizing the metal film in a further step. The method according to claim 3, comprising the further step of depositing an amorphous metal oxide layer over the metal film prior the step of thermally oxidizing the metal film. The method according to claim 3, wherein the metal cathode target is selected from the group consisting of titanium, zirconium, tantalum, hafnium, niobium, vanadium and mixtures thereof. The method of claim 4, wherein the amorphous metal oxide layer is deposited by sputtering and comprises the same metal as the underlying amorphous metal layer. The method of claim 4, wherein the amorphous metal oxide layer has a thickness in the range of 4 nm to 12 nm (40 to 120 Angstroms). The method of claims 2 or 5, wherein the metal cathode target is titanium. The method of claim 3, wherein the atmosphere in step (b) comprises argon and 2.5 to 10 percent oxygen, the amorphous metal film is an amorphous titanium film and in step (c) the amorphous titanium film is heated in air to a temperature of at least 400°C to effect complete oxidation resulting in a crystalline metal oxide film. The method according to any of the preceding claims 1 to 9, wherein the substrate is glass.

Inventors: ARBAB MEHRAN, FINLEY JAMES JOSEPH, ARBAB, MEHRAN
Applicants: PPG IND OHIO INC, PPG INDUSTRIES OHIO, INC.
Application year: 1994
Main classification: C23C14
IPC codes: C03C17, C23C14